NSR Query Results
Output year order : Descending NSR database version of March 18, 2024. Search: Author = M.Horoi Found 103 matches. Showing 1 to 100. [Next]2023HO04 Phys.Rev. C 107, 045501 (2023) Predicting the neutrinoless double-β-decay matrix element of 136Xe using a statistical approach RADIOACTIVITY 136Xe(2β-); calculated nuclear matrix elements (NMEs) of 0νββ-decay, probability distributions of NMEs calculated with SVD, jj55t and gcn5082 Hamiltonians. Statistical method based on Bayesian averaging model for analyzing the distribution and the theoretical uncertainty of the 0νββ decay NMEs. Obtained correlation matrix between 24 observables and defined the set of desired experimental precise values to reduce uncertainties in NMEs.
doi: 10.1103/PhysRevC.107.045501
2022CI08 J.Phys.(London) G49, 120502 (2022) V.Cirigliano, Z.Davoudi, J.Engel, R.J.Furnstahl, G.Hagen, U.Heinz, H.Hergert, M.Horoi, C.W.Johnson, A.Lovato, E.Mereghetti, W.Nazarewicz, A.Nicholson, T.Papenbrock, S.Pastore, M.Plumlee, D.R.Phillips, P.E.Shanahan, S.R.Stroberg, F.Viens, A.Walker-Loud, K.A.Wendt, S.M.Wild Towards precise and accurate calculations of neutrinoless double-beta decay RADIOACTIVITY 48Ca(2β-); calculated neutrinoless nuclear matrix elements using chiral-EFT interactions, EDF, IBM, QRPA, SM-pf, SM-sdpf, SM-MBPT, RSM, QMC+SM, IM-GCM, VS-IMSRG, CCSD, CCSD-T1.
doi: 10.1088/1361-6471/aca03e
2022HO16 Phys.Rev. C 106, 054302 (2022) Statistical analysis for the neutrinoless double-β-decay matrix element of 48Ca NUCLEAR STRUCTURE 48Ca, 48Ti; calculated levels, J, π, B(E2), occupation probabilities, Gamow-Teller strength, probability density functions (PDF) for observables. Interactive shell model in the fp-shell model space with FPD6, GXPF1A, and KB3G effective Hamiltonians. Comparison to experimental values. RADIOACTIVITY 48Ca(2β-); calculated nuclear matrix elements (NMEs) of 0νββ-decay and 2νββ, GT-strength, NME probability density function. Interactive shell model in the fp-shell model space with FPD6, GXPF1A, and KB3G effective Hamiltonians. Obtained correlation matrix between 24 observables and defined the set of desired experimental precise values to reduce uncertainties in NMEs.
doi: 10.1103/PhysRevC.106.054302
2021GA01 Nucl.Instrum.Methods Phys.Res. A985, 164603 (2021) P.Gastis, G.Perdikakis, G.P.A.Berg, A.C.Dombos, A.Estrade, A.Falduto, M.Horoi, S.N.Liddick, S.Lipschutz, S.Lyons, F.Montes, A.Palmisano, J.Pereira, J.S.Randhawa, T.Redpath, M.Redshaw, J.Schmitt, J.R.Sheehan, M.K.Smith, P.Tsintari, A.C.C.Villari, K.Wang, R.G.T.Zegers A technique for the study of (p, n) reactions with unstable isotopes at energies relevant to astrophysics NUCLEAR REACTIONS 1H(40Ar, n), E=3.52 MeV/nucleon; measured reaction products, En, In; deduced σ. Comparison with available data.
doi: 10.1016/j.nima.2020.164603
2020AH01 Phys.Rev. C 101, 035504 (2020) Interference effects for 0νββ decay in the left-right symmetric model RADIOACTIVITY 48Ca, 76Ge, 82Se, 124Sn, 130Te, 136Xe(2β-); calculated nuclear matrix elements (NMEs) from shell model and phase space factors (PSFs), interference coefficients for neutrinoless double beta (0νββ) decay rate for 0+ to 0+ transitions using the left-right symmetric model. Discussed variation of the interference effect with the Q values.
doi: 10.1103/PhysRevC.101.035504
2020HO04 Eur.Phys.J. A 56, 39 (2020) On the MSW-like neutrino mixing effects in atomic weak interactions and double beta decays
doi: 10.1140/epja/s10050-020-00042-x
2020RE12 Phys.Lett. B 809, 135702 (2020), Erratum Phys.Lett. B 820, 136532 (2021) B.M.Rebeiro, S.Triambak, P.E.Garrett, B.A.Brown, G.C.Ball, R.Lindsay, P.Adsley, V.Bildstein, C.Burbadge, A.Diaz Varela, T.Faestermann, D.L.Fang, R.Hertenberger, M.Horoi, B.Jigmeddorj, M.Kamil, K.G.Leach, P.Z.Mabika, J.C.Nzobadila Ondze, J.N.Orce, H.-F.Wirth Benchmarking 136Xe neutrinoless ββ decay matrix element calculations with the 138Ba(p, t) reaction NUCLEAR REACTIONS 138Ba(p, t), (p, p), E=23 MeV; measured reaction products, Ep, Ip; deduced σ(θ), neutrinoless ββ decay matrix elements.
doi: 10.1016/j.physletb.2020.135702
2019AY03 Phys.Rev.Lett. 123, 082501 (2019) Y.Ayyad, B.Olaizola, W.Mittig, G.Potel, V.Zelevinsky, M.Horoi, S.Beceiro Novo, M.Alcorta, C.Andreoiu, T.Ahn, M.Anholm, L.Atar, A.Babu, D.Bazin, N.Bernier, S.S.Bhattacharjee, M.Bowry, R.Caballero-Folch, M.Cortesi, C.Dalitz, E.Dunling, A.B.Garnsworthy, M.Holl, B.Kootte, K.G.Leach, J.S.Randhawa, Y.Saito, C.Santamaria, P.Siuryte, C.E.Svensson, R.Umashankar, N.Watwood, D.Yates Direct Observation of Proton Emission in 11Be RADIOACTIVITY 11Be(β-p) [from U(p, X), E=480 MeV]; measured decay products, Eβ, Iβ, Ep, Ip; deduced level energy, resonance parameters, J, π. Comparison with available data.
doi: 10.1103/PhysRevLett.123.082501
2018HO11 Phys.Rev. C 98, 035502 (2018) Shell model study of using an effective field theory for disentangling several contributions to neutrinoless double-β decay RADIOACTIVITY 48Ca, 76Ge, 82Se, 130Te, 136Xe(2β-); calculated 20 shell model nuclear matrix elements, Q values and nine phase space factors (PSFs) for 0νββ decay mode; deduced 12 lepton-number-violating (LNV) parameters corresponding to 12 0νββ decay mechanisms using limits on experimental half-lives, coupling limits including Majorana neutrino mass. Effective field theory approach, and beyond Standard Model physics for 0νββ decay.
doi: 10.1103/PhysRevC.98.035502
2018JI09 Phys.Rev. C 98, 064324 (2018) Neutrinoless double-β decay of 124Sn, 130Te, and 136Xe in the Hamiltonian-based generator-coordinate method RADIOACTIVITY 124Sn, 130Te, 136Xe(2β-); calculated matrix elements for 0νββ decay mode using generator-coordinate method (GCM) with realistic shell-model interactions. Comparison with shell-model calculations obtained by exactly diagonalizing the same effective Hamiltonian. NUCLEAR STRUCTURE 124Sn, 124,130Te, 130,136Xe, 136Ba; calculated ground state energies, low-lying 2+ and 4+ levels, B(E2) for the first 2+ states, occupancies of valence neutron and proton orbits using generator-coordinate method (GCM) with realistic shell-model interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.98.064324
2016HO03 Phys.Rev. C 93, 024308 (2016) Shell model predictions for 124Sn double-β decay RADIOACTIVITY 124Sn(2β-); calculated Gamow-Teller and Fermi nuclear matrix elements (NMEs), GT strengths, and half-lives for 2νββ and 0νββ decay modes using shell model. Comparison with existing calculations based on quasiparticle random-phase approximation (QRPA). 48Ca, 76Ge, 82Se, 124Sn, 130Te, 136Xe(2β-);reviewed calculated nuclear matrix elements (NMEs) for 0νββ decay mode using different nuclear structure methods for the light and heavy neutrino-exchange mechanisms. NUCLEAR STRUCTURE 124Sn, 124Te; calculated levels, J, π, B(E2) for first 2+ states, occupation probabilities, neutron- and proton-shell vacancies. 126,128Te; calculated B(E2) for first 2+ states. Comparison with experimental values.
doi: 10.1103/PhysRevC.93.024308
2016NE13 Adv.High Energy Phys. 2016, 1 (2016) An Effective Method to Accurately Calculate the Phase Space Factors for β-β-Decay RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 110Pd, 116Cd, 130Te, 136Xe, 150Nd(2β-); calculated phase factors taking into account the distorted Coulomb field of the daughter nucleus. Comparison with available data.
doi: 10.1155/2016/7486712
2016PR01 At.Data Nucl.Data Tables 107, 1 (2016), Erratum At.Data Nucl.Data Tables 114, 371 (2017) B.Pritychenko, M.Birch, B.Singh, M.Horoi Tables of E2 transition probabilities from the first 2+ states in even-even nuclei COMPILATION 4,6,8,10He, 6,8,10,12,14Be, 10,12,14,16,18,20C, 12,14,16,18,20,22,24,26O, 16,18,20,22,24,26,28,30,32Ne, 20,22,24,26,28,30,32,34,36,38Mg, 24,26,28,30,32,34,36,38,40,42Si, 28,30,32,34,36,38,40,42,44,46S, 32,34,36,38,40,42,44,46,48Ar, 36,38,40,42,44,46,48,50,52,54Ca, 42,44,46,48,50,52,54,56,58Ti, 46,48,50,52,54,56,58,60,62,64Cr, 48,50,52,54,56,58,60,62,64,66,68Fe, 52,54,56,58,60,62,64,66,68,70,72,74,76Ni, 60,62,64,66,68,70,72,74,76,78,80Zn, 62,64,66,68,70,72,74,76,78,80,82,84,86Ge, 66,68,70,72,74,76,78,80,82,84,86Se, 72,74,76,78,80,82,84,86,88,90,92,94,96Kr, 76,78,80,82,84,86,88,90,92,94,96,98,100,102Sr, 80,82,84,86,88,90,92,94,96,98,100,102,104,106,108Zr, 84,86,88,90,92,94,96,98,100,102,104,106,108,110Mo, 88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118Ru, 92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128Pd, 98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130Cd, 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138Te, 110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144Xe, 118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148Ba, 122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152Ce, 128,130,132,134,136,138,140,142,144,146,148,150,152,154,156Nd, 130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160Sm, 138,140,142,144,146,148,150,152,154,156,158,160,162,164Gd, 140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170Dy, 144Er, 148,150,152,154,156,158,160,162,164,166,168,170,172,174Er, 152,154,156,158,160,162,164,166,168,170,172,174,176,178Yb, 160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192W, 162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198Os, 168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204Pt, 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210Hg, 180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 206,208,210,212,214,216,218,220,222,224,226,228,230,232Ra, 214,216,218,220,222,224,226,228,230,232,234,236Th, 226,228,230,232,234,236,238,240,242U, 236,238,240,242,244,246Pu, 238,240,242,244,246,248,250Cm, 244,246,248,250,252Cf, 246,248Fm, 252,254,256Fm, 252,254No, 256Rf; compiled evaluated B(E2) values, T1/2, deformation parameters, first 2+ state energies in even-even nuclei. NUCLEAR STRUCTURE 6He, 10,12Be, 10,12,14,16,18,20C, 16,18,20,22O, 18,20,22,24,26,28,30Ne, 20,22,24,26,28,30,32,34Mg, 24,26,28,30,32,34,36,38,40Si, 30,32,34,36,38,40,42,44S, 32,34,36,38,40,42,44,46Ar, 38,40,42Ca, 46,48,50Ca, 42,44,46,48,50,52,54,56Ti, 46,48,50,52,54,56,58,60,62Cr, 50,52,54,56,58,60,62,64,66Fe, 54,56,58,60,62,64,66,68,70,72,74,76Ni, 62,64,66,68,70,72,74,76,78Zn, 104,106Sn; calculated transition energies, B(E2). Nuclear shell model.
doi: 10.1016/j.adt.2015.10.001
2016SE04 Phys.Rev. C 93, 044334 (2016) Shell-model calculation of neutrinoless double-β decay of 76Ge RADIOACTIVITY 76Ge(2β-); calculated nuclear matrix elements (NMEs) for 0νββ decay mode using a realistic shell-model approach beyond the closure approximation with realistic jj44 model space and JUN45 effective Hamiltonian. NUCLEAR STRUCTURE 76Ge, 76Se; calculated neutron occupancies of the p, f5/2 and g9/2 orbitals. 44,46,48Ca, 76Ge, 82Se; calculated optimal closure energies for GXPF1A, FPD6, and KB3G and JUN45 effective Hamiltonians. Comparison of occupation probabilities and Gamow-Teller strength with experimental data.
doi: 10.1103/PhysRevC.93.044334
2015BR15 Phys.Rev. C 92, 041301 (2015) Evaluation of the theoretical nuclear matrix elements for ββ decay of 76Ge RADIOACTIVITY 76Ge(2β-); calculated nuclear matrix elements (NMEs) for 2νββ and 0νββ decay modes using configuration-interaction (CI), quasiparticle random-phase approximation (QRPA), and interacting boson model methods. Comparison with experimental values.
doi: 10.1103/PhysRevC.92.041301
2015GA42 Phys.Rev. C 92, 064310 (2015) Variation after projection with a triaxially deformed nuclear mean field NUCLEAR STRUCTURE 20,22,24,26,28Ne, 24,26,28,30Mg, 28,30,32Si, 32,34S, 36Ar; calculated converged energies and associated shape parameters for even-even sd-shell nuclei with the USDB Hamiltonian. Variation after projection (VAP) calculations on spin, isospin, and mass number of a triaxially deformed Hartree-Fock-Bogoliubov vacuum state.
doi: 10.1103/PhysRevC.92.064310
2015NE03 Phys.Rev. C 91, 024309 (2015) Shell model studies of the 130Te neutrinoless double-β decay NUCLEAR STRUCTURE 130Te, 130,136Xe, 136Ba; calculated levels, J, π, GT strengths for 130Te to 130I and 136Xe to 136Cs transitions. 128,130Te, 130,132Xe; calculated neutron and proton shell vacancies, B(E2). Shell model calculations using SVD effective Hamiltonian. Comparison with available experimental values. RADIOACTIVITY 130Te, 136Xe(2β-); calculated GT strengths nuclear matrix elements (NME) for 2νββ and 0νββ decays for light and heavy neutrino exchanges. Shell model approach using a recently proposed effective Hamiltonian SVD, and jj55 model space. Comparison with calculations for double β decays of 48Ca, 76Ge, 82Se.
doi: 10.1103/PhysRevC.91.024309
2014BR22 Phys.Rev.Lett. 113, 262501 (2014) B.A.Brown, M.Horoi, R.A.Senkov Nuclear Structure Aspects of Neutrinoless Double-β Decay RADIOACTIVITY 76Ge, 48Ca, 82Se(2β-); calculated nuclear matrix elements as sums of products over the intermediate nucleus with two less nucleons; deduced the importance of the ground state of intermediate nucleus.
doi: 10.1103/PhysRevLett.113.262501
2014HA06 Phys.Rev. C 89, 034315 (2014) M.Haaranen, M.Horoi, J.Suhonen Shell-model study of the 4th- and 6th-forbidden β-decay branches of 48Ca RADIOACTIVITY 48Ca(β-), (2β-); calculated partial half-lives for 4th and 6th-forbidden β decays to 6+, 5+ and 4+ states in 48Sc. Competition between single β decay and 2νββ decay branches. Shell-model calculations using GXPF1A effective interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.034315
2014KW04 Phys.Rev. C 89, 045502 (2014) A.A.Kwiatkowski, T.Brunner, J.D.Holt, A.Chaudhuri, U.Chowdhury, M.Eibach, J.Engel, A.T.Gallant, A.Grossheim, M.Horoi, A.Lennarz, T.D.Macdonald, M.R.Pearson, B.E.Schultz, M.C.Simon, R.A.Senkov, V.V.Simon, K.Zuber, J.Dilling New determination of double-β-decay properties on 48Ca High-precision Qββ-value measurement and improved nuclear matrix element calculations ATOMIC MASSES 48Ca, 48Ti; measured cyclotron-frequencies, resonances using TITAN system consisting of radio frequency quadrupole (RFQ) beam cooler and buncher, an electron beam ion trap (EBIT), and a Penning trap (MPET) at ISAC-TRIUMF facility; deduced Q value for double β decay of 48Ti. Comparison with previous measurements and atomic mass evaluations (AME-2003 and AME-2012). RADIOACTIVITY 48Ca(2β-); measured precise Q-value using TITAN system at ISAC-TRIUMF facility; calculated ββ nuclear matrix element by including effects of levels outside the valence space in a shell-model; discussed case for a new experiment on double-beta decay of 48Ca.
doi: 10.1103/PhysRevC.89.045502
2014PR06 Nucl.Data Sheets 120, 112 (2014) B.Pritychenko, M.Birch, M.Horoi, B.Singh B(E2) Evaluation for 0+1 → 2+1 Transitions in Even-Even Nuclei COMPILATION 46,48Ca, 46,48Ti, 70Zn, 70,76Ge, 76,80,82Se, 80,82,86Kr, 86Sr, 94,96Zr, 94,96,100Mo, 100,104Ru, 104,110Pd, 110,114,116Cd, 114,116,122,124Sn, 122,124,128,130Te, 128,130,134,136Xe, 134,136Ba; compiled evaluated B(E2) values, deformation parameters, first 2+ state energies for 2β-decay candidates.
doi: 10.1016/j.nds.2014.07.021
2014SA46 Phys.Lett. B 736, 137 (2014) A.Sanetullaev, M.B.Tsang, W.G.Lynch, Jenny Lee, D.Bazin, K.P.Chan, D.Coupland, V.Henzl, D.Henzlova, M.Kilburn, A.M.Rogers, Z.Y.Sun, M.Youngs, R.J.Charity, L.G.Sobotka, M.Famiano, S.Hudan, D.Shapira, W.A.Peters, C.Barbieri, M.Hjorth-Jensen, M.Horoi, T.Otsuka, T.Suzuki, Y.Utsuno Neutron spectroscopic factors of 55Ni hole-states from image transfer reactions NUCLEAR REACTIONS 1H(56Ni, d), E=37 MeV/nucleon; measured reaction products; deduced spectroscopic factors, J, π, σ(θ). Comparison with shell model calculations.
doi: 10.1016/j.physletb.2014.07.003
2014SE10 Phys.Rev. C 89, 054304 (2014) R.A.Sen'kov, M.Horoi, B.A.Brown Neutrinoless double-β decay of 82Se in the shell model: Beyond the closure approximation RADIOACTIVITY 82Se(2β-); calculated nuclear matrix elements for neutrinoless double-beta decay (0νββ). Shell-model techniques using CD-Bonn-, Miller-Spencer-, and AV18-based short-range correlation (SRC) methods. Comparison with other theoretical calculations. Relevance to SuperNEMO experiment.
doi: 10.1103/PhysRevC.89.054304
2014SE21 Phys.Rev. C 90, 051301 (2014) Accurate shell-model nuclear matrix elements for neutrinoless double-β decay RADIOACTIVITY 76Ge(2β-); calculated nuclear matrix elements (NMEs), and average closure energies for neutrinoless double-β decay using realistic shell-model approach beyond closure approximation. 44,46,48Ca, 76Ge, 82Ge(2β-); calculated optimal closure energies for GXPF1A, FPD6, and KB3G for Ca and JUN45 for Ge and Se isotopes.
doi: 10.1103/PhysRevC.90.051301
2013BO19 Comput.Phys.Commun. 184, 085101 (2013) S.Bogner, A.Bulgac, J.Carlson, J.Engel, G.Fann, R.J.Furnstahl, S.Gandolfi, G.Hagen, M.Horoi, C.Johnson, M.Kortelainen, E.Lusk, P.Maris, H.Nam, P.Navratil, W.Nazarewicz, E.Ng, G.P.A.Nobre, E.Ormand, T.Papenbrock, J.Pei, S.C.Pieper, S.Quaglioni, K.J.Roche, J.Sarich, N.Schunck, M.Sosonkina, J.Terasaki, I.Thompson, J.P.Vary, S.M.Wild Computational nuclear quantum many-body problem: The UNEDF project NUCLEAR REACTIONS 3He(d, p), 7Be(p, γ), E<1MeV; 172Yb, 188Os, 238U(γ, X), E<24 MeV; calculated σ. Comparison with experimental data. NUCLEAR STRUCTURE 100Zr; calculated quadrupole deformation parameter, radii, neutron separation energy.
doi: 10.1016/j.cpc.2013.05.020
2013HO03 Phys.Rev. C 87, 014320 (2013) Shell model analysis of competing contributions to the double-β decay of 48Ca RADIOACTIVITY 48Ca(2β-); calculated two-neutrino and neutrinoless 2β- nuclear matrix elements, T1/2, prediction for transition to the first excited 0+ state using shell-model calculations.
doi: 10.1103/PhysRevC.87.014320
2013HO11 Phys.Rev.Lett. 110, 222502 (2013) Shell-Model Analysis of the 136Xe Double Beta Decay Nuclear Matrix Elements RADIOACTIVITY 136Xe(2β-); calculated neutrinoless mode nuclear matrix elements; deduced importance of nuclear orbitals necessary for a good description of the Gamow-Teller strength. Shell model analysis, comparison with available data.
doi: 10.1103/PhysRevLett.110.222502
2013LU10 Phys.Rev. C 88, 017604 (2013) F.Lu, J.Lee, M.B.Tsang, D.Bazin, D.Coupland, V.Henzl, D.Henzlova, M.Kilburn, W.G.Lynch, A.M.Rogers, A.Sanetullaev, Z.Y.Sun, M.Youngs, R.J.Charity, L.G.Sobotka, M.Famiano, S.Hudan, M.Horoi, Y.L.Ye Neutron-hole states in 45Ar from 1H(46Ar, d)45Ar reactions NUCLEAR REACTIONS 1H(46Ar, d), E=33 MeV/nucleon; measured E(d), I(d), σ(θ). Radioactive secondary beam of 46Ar produced in the Coupled Cyclotron facility at NSCL. 45Ar; deduced levels, J, π, L-transfer, spectroscopic factors. ADWA analysis. Comparison with spectroscopic factors determined in 2H(44Ar, p)45Ar reaction, and with shell-model calculations.
doi: 10.1103/PhysRevC.88.017604
2013SE22 Phys.Rev. C 88, 064312 (2013) Neutrinoless doubleβ in the shell model: Closure versus nonclosure approximation RADIOACTIVITY 48Ca(2β-); calculated the 0νββ nuclear matrix elements (NMEs) using closure approximation, a nonclosure approach, and a combined new method within shell model. 44,46Ca; calculated closure NME for fictitious 0νββ decay.
doi: 10.1103/PhysRevC.88.064312
2012BA33 Phys.Rev. C 86, 015806 (2012), Erratum Phys.Rev. C 86, 039901 (2012) A.Banu, F.Carstoiu, N.L.Achouri, W.N.Catford, M.Chartier, B.Fernandez-Dominguez, M.Horoi, B.Laurent, N.A.Orr, S.Paschalis, N.Patterson, B.Pietras, B.T.Roeder, P.Roussel-Chomaz, J.S.Thomas, L.Trache, R.E.Tribble One-proton breakup of 24Si and the 23Al(p, γ)24Si reaction in type I x-ray bursts NUCLEAR REACTIONS 12C(24Si, X)23Al, [24Si secondary beam from C(32S, X), E=95 MeV/nucleon primary reaction], E=61 MeV/nucleon; measured fragment spectra, σ, inclusive longitudinal momentum distribution, time-of-flight of 23Al fragments using SPEG spectrograph at GANIL; deduced spectroscopic factors, asymptotic normalization coefficient (ANC). Glauber-type analysis. Comparison with large-scale shell model calculations. 23Al(p, γ)24Si, E<1 MeV; deduced stellar reaction rates. Discussed astrophysical significance of 23Al(p, γ)24Si in type I x-ray bursts (XRB) nucleosynthesis. Waiting-point nuclei and relevance to 22Na abundance and sequential 2p capture on 22Mg at high temperature.
doi: 10.1103/PhysRevC.86.015806
2012BA46 J.Phys.:Conf.Ser. 337, 012059 (2012) A.Banu, F.Carstoiu, W.N.Catford, B.Fernandez-Dominguez, M.Horoi, N.A.Orr, B.T.Roeder, P.Roussel-Chomaz, L.Trache, R.E.Tribble Direct radiative proton capture 23Al(p, γ)24Si studied via one-proton nuclear breakup of 24Si NUCLEAR REACTIONS 12C(24Si, p23Al), E=20-60 MeV/nucleon; measured Eγ, Iγ, (fragment)γ-coin, reaction products using SPEG energy-loss spectrometer; deduced 23Al momentum distribution; calculated 23Al momentum distribution using Glauber-type approach.
doi: 10.1088/1742-6596/337/1/012059
2012DI04 Phys.Rev. C 85, 034311 (2012) E.S.Diffenderfer, L.T.Baby, D.Santiago-Gonzalez, N.Ahsan, A.Rojas, A.Volya, I.Wiedenhover, A.H.Wuosmaa, M.P.Carpenter, R.V.F.Janssens, C.J.Lister, M.Devlin, D.G.Sarantites, L.G.Sobotka, Y.Utsuno, M.Horoi High-spin spectrum of 24Mg studied through multiparticle angular correlations NUCLEAR REACTIONS 12C(16O, α)24Mg, E=62, 68 MeV; measured Eα, Iα, αγ-coin, αγ(θ), αγγ(θ) using Gammasphere array. Experiments carried out at ANL and FSU facilities. 24Mg; deduced levels, J, π, configurations. Comparison with previous studies and shell model calculations.
doi: 10.1103/PhysRevC.85.034311
2012NE11 Phys.Rev. C 86, 067304 (2012) Fast, efficient calculations of the two-body matrix elements of the transition operators for neutrinoless double-β decay RADIOACTIVITY 48Ca, 82Se(2β-); calculated two-body matrix elements (TBME) of neutrinoless double beta (0νββ) decay transition operator using a new, and fast algorithm.
doi: 10.1103/PhysRevC.86.067304
2012PR08 At.Data Nucl.Data Tables 98, 798 (2012) B.Pritychenko, J.Choquette, M.Horoi, B.Karamy, B.Singh An update of the B(E2) evaluation for 0+1 → 2+1 transitions in even-even nuclei near N ∼ Z ∼ 28 COMPILATION 46,48,50,52,54,56,58,60,62,64Cr, 48,50,52,54,56,58,60,62,64,66,68Fe, 54,56,58,60,62,64,66,68,70,72,74,76Ni, 60,62,64,66,68,70,72,74,76,78,80Zn; compiled evaluated and experimental B(E2) values and transition energies. NUCLEAR STRUCTURE 46,48,50,52,54,56,58,60,62Cr, 50,52,54,56,58,60,62,64Fe, 54,56,58,60,62,64,66,68,70,72,74,76Ni, 62,64,66,68,70,72,74,76,78Zn; calculated B(E2) values, transition energies. Nuclear shell model, GXPF1A and JUN45 effective interactions.
doi: 10.1016/j.adt.2012.06.004
2011BA27 Phys.Rev. C 84, 015803 (2011) A.Banu, L.Trache, F.Carstoiu, N.L.Achouri, A.Bonaccorso, W.N.Catford, M.Chartier, M.Dimmock, B.Fernandez-Dominguez, M.Freer, L.Gaudefroy, M.Horoi, M.Labiche, B.Laurent, R.C.Lemmon, F.Negoita, N.A.Orr, S.Paschalis, N.Patterson, E.S.Paul, M.Petri, B.Pietras, B.T.Roeder, F.Rotaru, P.Roussel-Chomaz, E.Simmons, J.S.Thomas, R.E.Tribble Structure of 23Al from the one-proton breakup reaction and astrophysical implications NUCLEAR REACTIONS 12C(23Al, 22Mg), [23Al secondary beam from C(32S, X)E=95 MeV/nucleon primary reaction], E=57 MeV/nucleon; measured fragment spectra, inclusive and exclusive longitudinal momentum distributions, and widths, Eγ, (fragment)γ-coin. 22Mg; deduced levels, J, π, σ, spectroscopic factors, asymptotic normalization coefficients. 23Al; deduced g.s. Jπ, configuration mixing. Comparison with Glauber and large-scale shell model calculations. 22Mg(p, γ)23Al, E<1 MeV; deduced stellar reaction rates; discussed astrophysical significance of 22Na nucleosynthesis in ONe novae.
doi: 10.1103/PhysRevC.84.015803
2011GA22 Phys.Rev. C 83, 057303 (2011) Z.-C.Gao, M.Horoi, Y.S.Chen, Y.J.Chen, Tuya Can one identify the intrinsic structure of the yrast states in 48Cr after the backbending? NUCLEAR STRUCTURE 48Cr; calculated levels, J, π, B(E2), configurations for yrast states using projected configuration interaction (PCI) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.057303
2010HO02 Phys.Rev. C 81, 024321 (2010) Shell model analysis of the neutrinoless double-β decay of 48Ca RADIOACTIVITY 48Ca(2β-); calculated nuclear matrix elements for neutrinoless double-β decay using large-scale shell model. NUCLEAR STRUCTURE 48Ca, 48Ti; calculated neutron and proton occupation probabilities, and nuclear matrix elements for double-β decay using large-scale shell model.
doi: 10.1103/PhysRevC.81.024321
2010HO05 Phys.Rev. C 81, 034306 (2010) Random interactions explore the nuclear landscape: Predominance of prolate nuclear deformations
doi: 10.1103/PhysRevC.81.034306
2010PE15 Phys.Rev. C 82, 064305 (2010) S.M.Perez, W.A.Richter, B.A.Brown, M.Horoi Magnetic moments of T=3/2 mirror pairs NUCLEAR MOMENTS 43V, 43Ca, 45Sc, 45Cr, 47Mn, 47Ti, 49Fe, 49V, 51Co, 51Cr, 53Ni, 53Mn; analyzed magnetic moments, γp and γn values of T=3/2 proton-rich nuclei in fp shell by using experimental values for their neutron-rich mirror nuclei. 19Na, 19O, 21F, 21Mg, 23Al, 23Ne, 25Na, 25Si, 27P, 27Mg, 29Al, 29S, 31Cl, 31Si, 33P, 33Ar, 35K, 35S, 37Cl, 37Ca; analyzed gp and γn values of T=3/2 mirror nuclei in sd shell. Shell model calculations.
doi: 10.1103/PhysRevC.82.064305
2010SC20 Europhys.Lett. 91, 52001 (2010) Improved accuracy moments method for spin-dependent shell model nuclear level densities NUCLEAR STRUCTURE 48,50Ti, 50,52Cr, 64Ge; calculated nuclear level densities, positive- and negative-parity states.
doi: 10.1209/0295-5075/91/52001
2010SE09 Phys.Rev. C 82, 024304 (2010) High-performance algorithm to calculate spin- and parity-dependent nuclear level densities NUCLEAR STRUCTURE 28Si, 52Fe, 52Cr, 60Zn, 64Ge, 68Se, 70Br; calculated spin and parity dependent shell model nuclear level density using moments method in the proton-neutron formalism. Comparisons with exact shell-model calculations. Calculations performed on FRANKLIN supercomputer.
doi: 10.1103/PhysRevC.82.024304
2009GA03 Phys.Rev. C 79, 014311 (2009) Angular momentum projected configuration interaction with realistic Hamiltonians NUCLEAR STRUCTURE 28Si; calculated ground-state energies. 20Ne, 24Mg, 28Si, 36Ar; calculated deformation HF energies. 24Mg, 28Si, 48Cr, 56Ni; calculated quadrupole moments, B(E2). 24Mg, 28Si, 48Cr; calculated levels, J, π. 52Fe, 56Ni; calculated yrast band energies using full configuration interaction method.in sd-pf shell space.
doi: 10.1103/PhysRevC.79.014311
2009GA29 Phys.Rev. C 80, 034325 (2009) Improved basis selection for the projected configuration interaction method applied to medium-heavy nuclei NUCLEAR STRUCTURE 56Ni, 68,70,76Se, 76Ge; calculated level energies using Projection Configuration Interaction (PCI) and full configuration interaction (CI) approaches. 76Ge, 76Se; calculated low-lying 0+ states.
doi: 10.1103/PhysRevC.80.034325
2009HI08 Phys.Rev. C 80, 014313 (2009) G.W.Hitt, R.G.T.Zegers, Sam M.Austin, D.Bazin, A.Gade, D.Galaviz, C.J.Guess, M.Horoi, M.E.Howard, W.D.M.Rae, Y.Shimbara, E.E.Smith, C.Tur Gamow-Teller transitions to 64Cu measured with the 64Zn(t, 3He) reaction NUCLEAR REACTIONS 64Zn(t, 3He), E=115 MeV/nucleon; measured particle spectra, σ(θ) and Gamow-Teller strength distributions; deduced electron capture rate on 64Zn as a function of stellar temperature. Comparison with shell model calculations and experimental data from 64Zn(d, 2He) reaction.
doi: 10.1103/PhysRevC.80.014313
2009LE14 Phys.Rev. C 79, 054611 (2009) J.Lee, M.B.Tsang, W.G.Lynch, M.Horoi, S.C.Su Neutron spectroscopic factors of Ni isotopes from transfer reactions NUCLEAR REACTIONS 58,60,61,62,64Ni(d, p), (p, d), E not given; analyzed experimental angular distributions using adiabatic distorted wave approximation (ADWA). 57,58,59,60,61,62,63,64Ni; deduced spectroscopic factors for ground and excited states. Comparison with large basis shell-model calculations.
doi: 10.1103/PhysRevC.79.054611
2009TS01 Phys.Rev.Lett. 102, 062501 (2009) M.B.Tsang, J.Lee, S.C.Su, J.Y.Dai, M.Horoi, H.Liu, W.G.Lynch, S.Warren Survey of Excited State Neutron Spectroscopic Factors for Z = 8-28 Nuclei NUCLEAR STRUCTURE 17,18O, 21Ne, 24Na, 26,27Mg, 29,30,31Si, 33,35S, 41,43,45,47,49Ca, 47,49,51Ti, 51,53,55Cr, 57,59,61,62,63,65Ni; calculated excited state neutron spectroscopic factors.
doi: 10.1103/PhysRevLett.102.062501
2008GO19 Phys.Rev.Lett. 101, 052501 (2008) J.R.Gour, M.Horoi, P.Piecuch, B.A.Brown Coupled-Cluster and Configuration-Interaction Calculations for Odd-A Heavy Nuclei NUCLEAR STRUCTURE 55,57Ni; calculated binding energies, and low-lying level energies using Coupled-Cluster and Configuration-Interaction.
doi: 10.1103/PhysRevLett.101.052501
2008MA01 Phys.Rev. C 77, 014313 (2008) P.F.Mantica, R.Broda, H.L.Crawford, A.Damaske, B.Fornal, A.A.Hecht, C.Hoffman, M.Horoi, N.Hoteling, R.V.F.Janssens, J.Pereira, J.S.Pinter, J.B.Stoker, S.L.Tabor, T.Sumikama, W.B.Walters, X.Wang, S.Zhu β decay of neutron-rich 53-56Ca RADIOACTIVITY 53,54,55,56Ca(β-) [from 9Be(76Ge, X), E=140 MeV/nucleon; measured Eγ, Iγ, βγ-coin, half-lives. 54Ca; deduced Iβ, logft. 54Sc; levels, J, π, half-lives, B(M1), B(E2), comparison with calculations. NUCLEAR REACTIONS 9Be(76Ge, X)49Cl/50Ar/51Ar/52K/53K/54K/53Ca/54Ca/55Ca/56Ca/55Sc/56Sc/57Sc/57Ti/58Ti/59Ti/60V, E=140 MeV/nucleon; measured reaction yields.
doi: 10.1103/PhysRevC.77.014313
2008PE13 Phys.Rev. C 77, 064311 (2008) S.M.Perez, W.A.Richter, B.A.Brown, M.Horoi Correlations between magnetic moments and β decays of mirror nuclei NUCLEAR STRUCTURE 11B, 11,13C, 13,15N, 15,17O, 17,19F, 19,21Ne, 21,23Na, 23,25Mg, 25,27Al, 27,29Si, 29,31P, 31,33S, 33,35Cl, 35,37Ar, 37,39K, 39,41Ca, 41,43Sc, 43,45Ti, 45,47V, 47,49Cr, 49,51Mn, 51,53Fe, 53,55Co, 55,57Ni, 57Cu; calculated magnetic moments, β-decay half-lives, gyromagnetic ratios.
doi: 10.1103/PhysRevC.77.064311
2007CA35 Phys.Lett. B 652, 169 (2007); Addendum Phys.Lett. B 656, 272 (2007) C.M.Campbell, N.Aoi, D.Bazin, M.D.Bowen, B.A.Brown, J.M.Cook, D.-C.Dinca, A.Gade, T.Glasmacher, M.Horoi, S.Kanno, T.Motobayashi, L.A.Riley, H.Sagawa, H.Sakurai, K.Starosta, H.Suzuki, S.Takeuchi, J.R.Terry, K.Yoneda, H.Zwahlen Quadrupole collectivity in silicon isotopes approaching neutron number N=28 NUCLEAR REACTIONS 1H(36Si, 36Si'), E < 140 MeV/nucleon; 1H(38Si, 38Si'), E < 140 MeV/nucleon; 1H(40Si, 40Si'), E < 140 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coinc, inelastic proton scattering cross sections. 36,38,40Si deduced quadrupole deformation parameters.
doi: 10.1016/j.physletb.2007.07.005
2007HO05 Phys.Rev.Lett. 98, 112501 (2007) M.Horoi, J.R.Gour, M.Wloch, M.D.Lodriguito, B.A.Brown, P.Piecuch Coupled-Cluster and Configuration-Interaction Calculations for Heavy Nuclei NUCLEAR STRUCTURE 56Ni; calculated level energies, J, π, configurations. Comparison of coupled-cluster and configuration-interaction results.
doi: 10.1103/PhysRevLett.98.112501
2007HO07 Phys.Rev. C 75, 034303 (2007) Shell-model calculations of two-neutrino double-β decay rates of 48Ca with the GXPF1A interaction NUCLEAR STRUCTURE 48Ca; calculated 2νββ-decay matrix elements, T1/2 for decay to ground and excited states. Shell model approach. RADIOACTIVITY 48Ca(2β-); calculated 2νββ-decay matrix elements, T1/2 for decay to ground and excited states. Shell model approach.
doi: 10.1103/PhysRevC.75.034303
2007HO10 Phys.Rev. C 75, 054303 (2007) Pairing phase transitions in nuclear wave functions NUCLEAR STRUCTURE 24Mg, 28Si; calculated pairing correlator in sd shell model.
doi: 10.1103/PhysRevC.75.054303
2007HO12 Phys.Rev.Lett. 98, 262503 (2007) Exact Removal of the Center-of-Mass Spurious States from Level Densities
doi: 10.1103/PhysRevLett.98.262503
2007LI84 Eur.Phys.J. Special Topics 150, 135 (2007) S.N.Liddick, P.F.Mantica, R.V.F.Janssens, B.A.Brown, M.P.Carpenter, A.D.Davies, M.Honma, M.Horoi, T.Mizusaki, A.C.Morton, W.F.Mueller, T.Otsuka, J.Pavan, H.Schatz, A.Stolz, S.L.Tabor, B.E.Tomlin, M.Wiedeking Beta-delayed γ-ray studies of πf7/2 - νpf shell nuclei
doi: 10.1140/epjst/e2007-00286-4
2007ST16 Phys.Rev.Lett. 99, 042503 (2007) K.Starosta, A.Dewald, A.Dunomes, P.Adrich, A.M.Amthor, T.Baumann, D.Bazin, M.Bowen, B.A.Brown, A.Chester, A.Gade, D.Galaviz, T.Glasmacher, T.Ginter, M.Hausmann, M.Horoi, J.Jolie, B.Melon, D.Miller, V.Moeller, R.P.Norris, T.Pissulla, M.Portillo, W.Rother, Y.Shimbara, A.Stolz, C.Vaman, P.Voss, D.Weisshaar, V.Zelevinsky Shape and Structure of N=Z 64Ge: Electromagnetic Transition Rates from the Application of the Recoil Distance Method to a Knockout Reaction NUCLEAR REACTIONS 93Nb(65Ge, n), (63Zn, n), E not given; measured Eγ, Iγ and transition rates using recoil distance method. 64Ge, 62Zn deduced B(E2) and lifetimes.
doi: 10.1103/PhysRevLett.99.042503
2007VA22 Phys.Rev.Lett. 99, 162501 (2007) C.Vaman, C.Andreoiu, D.Bazin, A.Becerril, B.A.Brown, C.M.Campbell, A.Chester, J.M.Cook, D.C.Dinca, A.Gade, D.Galaviz, T.Glasmacher, M.Hjorth-Jensen, M.Horoi, D.Miller, V.Moeller, W.F.Mueller, A.Schiller, K.Starosta, A.Stolz, J.R.Terry, A.Volya, V.Zelevinsky, H.Zwahlen Z=50 Shell Gap near 100Sn from Intermediate-Energy Coulomb Excitations in Even-Mass 106-112Sn Isotopes NUCLEAR REACTIONS 197Au(106Sn, 106Sn'), (108Sn, 108Sn'), (110Sn, 110sn'), (112Sn, 112Sn'), E=78-81 MeV; measured Eγ, Iγ, (particle)γ-coinc from projectile coulomb excitation. 106,108,110,112Sn deduced B(E2).
doi: 10.1103/PhysRevLett.99.162501
2006CA26 Phys.Rev.Lett. 97, 112501 (2006) C.M.Campbell, N.Aoi, D.Bazin, M.D.Bowen, B.A.Brown, J.M.Cook, D.-C.Dinca, A.Gade, T.Glasmacher, M.Horoi, S.Kanno, T.Motobayashi, W.F.Mueller, H.Sakurai, K.Starosta, H.Suzuki, S.Takeuchi, J.R.Terry, K.Yoneda, H.Zwahlen Measurement of Excited States in 40Si and Evidence for Weakening of the N = 28 Shell Gap NUCLEAR REACTIONS 1H(40Si, 40Si'), (42P, 40SiX), E ≈ 80 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin. 40Si deduced excited states energies. Comparison with model predictions.
doi: 10.1103/PhysRevLett.97.112501
2006FO13 Phys.Rev. C 74, 034308 (2006) N.Fotiades, A.F.Lisetskiy, J.A.Cizewski, R.Krucken, R.M.Clark, P.Fallon, I.Y.Lee, A.O.Macchiavelli, J.A.Becker, B.A.Brown, M.Horoi, W.Younes First observation of high-spin states in 83Se NUCLEAR REACTIONS 208Pb(18O, F)83Se/138Ba/139Ba/140Ba, E=91 MeV; measured Eγ, Iγ, γγ-coin. 83Se deduced high-spin levels, J, π, configurations. Gammasphere array.
doi: 10.1103/PhysRevC.74.034308
2006GA31 Phys.Rev. C 74, 034322 (2006) A.Gade, B.A.Brown, D.Bazin, C.M.Campbell, J.A.Church, D.C.Dinca, J.Enders, T.Glasmacher, M.Horoi, Z.Hu, K.W.Kemper, W.F.Mueller, T.Otsuka, L.A.Riley, B.T.Roeder, T.Suzuki, J.R.Terry, K.L.Yurkewicz, H.Zwahlen Evolution of the E(1/2+1) - E(3/2+1) energy spacing in odd-mass K, Cl, and P isotopes for N = 20-28 NUCLEAR REACTIONS H, C(46Ar, X)43Cl/45Cl, E=76.4 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin. 45Cl deduced level energy. NUCLEAR STRUCTURE 35,37,39,41,43P, 37,39,41,43,45Cl, 39,41,43,45,47K; analyzed level energies, splitting.
doi: 10.1103/PhysRevC.74.034322
2006GA35 Phys.Rev. C 74, 047302 (2006) A.Gade, R.V.F.Janssens, D.Bazin, B.A.Brown, C.M.Campbell, M.P.Carpenter, J.M.Cook, A.N.Deacon, D.-C.Dinca, S.J.Freeman, T.Glasmacher, M.Horoi, B.P.Kay, P.F.Mantica, W.F.Mueller, J.R.Terry, J.A.Tostevin, S.Zhu One-neutron knockout in the vicinity of the N = 32 sub-shell closure: 9Be(57Cr, 56Cr+γ)X NUCLEAR REACTIONS 9Be(57Cr, 56CrX), E=77 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin, parallel momentum distribution; deduced σ. 56Cr deduced levels, spectroscopic factors.
doi: 10.1103/PhysRevC.74.047302
2006HO07 Phys.Rev. C 73, 061305 (2006); Erratum Phys.Rev. C 74, 059904 (2006) M.Horoi, B.A.Brown, T.Otsuka, M.Honma, T.Mizusaki Shell model analysis of the 56Ni spectrum in the full pf model space NUCLEAR STRUCTURE 56Ni; calculated levels, J, π, B(E2), rotational bands. Shell model, comparison with data.
doi: 10.1103/PhysRevC.73.061305
2006HO10 Chem.Phys.Lett. 427, 147 (2006) Signature of shape transition and shape coexistence in mesoscopic systems NUCLEAR STRUCTURE Sm; analyzed binding energies, shape transition and shape coexistence effects.
doi: 10.1016/j.cplett.2006.06.017
2006LI15 Phys.Rev. C 73, 044322 (2006) S.N.Liddick, P.F.Mantica, B.A.Brown, M.P.Carpenter, A.D.Davies, M.Horoi, R.V.F.Janssens, A.C.Morton, W.F.Mueller, J.Pavan, H.Schatz, A.Stolz, S.L.Tabor, B.E.Tomlin, M.Wiedeking Half-life and spin of 60Mng RADIOACTIVITY 60Cr, 60Mn(β-) [from Be(86Kr, X) and subsequent decay]; measured β-delayed Eγ, Iγ, T1/2; deduced log ft. 60Fe, 60Mn deduced levels J, π, configurations, β-feeding intensities. Comparison with shell model predictions.
doi: 10.1103/PhysRevC.73.044322
2006WA18 Phys.Rev. C 74, 014605 (2006) R.E.Warner, F.Carstoiu, J.A.Brown, F.D.Becchetti, D.A.Roberts, B.Davids, A.Galonsky, R.M.Ronningen, M.Steiner, M.Horoi, J.J.Kolata, A.Nadasen, C.Samanta, J.Schwarzenberg, K.Subotic Reaction and proton-removal cross sections of 6Li, 7Be, 10B, 9, 10, 11C, 12N, 13, 15O, and 17Ne on Si at 15 to 53 MeV/nucleon NUCLEAR REACTIONS Si(6Li, X), (7Be, X), (10B, X), (9C, X), (10C, X), (11C, X), (12N, X), (13O, X), (15O, X), (17Ne, X), E=15-53 MeV/nucleon; measured reaction and proton-removal σ. 6Li, 7Be, 10B, 9,10,11C, 12N, 13,15O, 17Ne deduced radii. Comparison with Glauber model predictions.
doi: 10.1103/PhysRevC.74.014605
2005AS04 Phys.Rev. C 72, 024314 (2005) N.I.Ashwood, M.Freer, D.J.Millener, N.A.Orr, F.Carstoiu, S.Ahmed, J.C.Angelique, V.Bouchat, W.N.Catford, N.M.Clarke, N.Curtis, F.Hanappe, M.Horoi, Y.Kerckx, J.L.Lecouey, F.M.Marques, T.Materna, G.Normand, S.Pain, N.Soic, C.Timis, A.Unshakova, V.A.Ziman High-energy two-neutron removal from 10Be NUCLEAR REACTIONS 12C(10Be, 2α), (10Be, n2α), E=30 MeV/nucleon; measured En, Eα, relative energy spectra, σ(E). 8,9Be deduced levels, J, π. Kinematically complete measurement.
doi: 10.1103/PhysRevC.72.024314
2005HO23 Nucl.Phys. A758, 138c (2005) Can one measure the temperature dependence of the fusion reaction rates? NUCLEAR REACTIONS 2H(t, α), 1H(7Li, α), 7Li(p, α), E=low; calculated enhancement factors vs temperature for astrophysical reaction rates.
doi: 10.1016/j.nuclphysa.2005.05.028
2005HO24 Nucl.Phys. A758, 142c (2005) M.Horoi, M.Ghita, V.Zelevinsky Comparison of approaches for spin- and parity-dependent shell model nuclear level density NUCLEAR STRUCTURE 28Si; calculated spin- and parity-dependent shell model level densities. Several approaches compared.
doi: 10.1016/j.nuclphysa.2005.05.029
2005LI53 Phys.Rev. C 72, 054321 (2005) S.N.Liddick, P.F.Mantica, R.Broda, B.A.Brown, M.P.Carpenter, A.D.Davies, B.Fornal, M.Horoi, R.V.F.Janssens, A.C.Morton, W.F.Mueller, J.Pavan, H.Schatz, A.Stolz, S.L.Tabor, B.E.Tomlin, M.Wiedeking β-decay of odd-A 57Ti and 59V RADIOACTIVITY 57Ti, 59V, 59Cr(β-) [from Be(86Kr, X)]; measured β-delayed Eγ, Iγ, γγ-coin, T1/2; deduced log ft. 57V, 59Cr, 59Mn deduced levels, β-feeding intensities, deformation. Comparison with shell-model predictions.
doi: 10.1103/PhysRevC.72.054321
2005LI54 Eur.Phys.J. A 25, Supplement 1, 95 (2005) A.F.Lisetskiy, B.A.Brown, M.Horoi Exotic nuclei near 78Ni in a shell model approach NUCLEAR STRUCTURE 70,72,74,76Ni, 92Mo, 94Ru, 96Pd, 98Cd; calculated B(E2). 57,59,61,63,65,67,69,71,73,75,77,79Cu; calculated level energies. Shell model, comparison with data.
doi: 10.1140/epjad/i2005-06-158-1
2004HO10 Phys.Rev. C 69, 041307 (2004) M.Horoi, M.Ghita, V.Zelevinsky Fixed spin and parity nuclear level density for restricted shell model configurations
doi: 10.1103/PhysRevC.69.041307
2004HO12 J.Phys.(London) G30, 945 (2004) Scaling behaviour in cluster decay RADIOACTIVITY 224Th(16O); 224Th, 221Ra, 222,223Ac(14C); 221Ra, 222Ac(12C); 223Ac(15N); calculated cluster decay T1/2, Q-values, scaling behaviour.
doi: 10.1088/0954-3899/30/7/010
2004LI64 Phys.Rev. C 70, 044314 (2004) A.F.Lisetskiy, B.A.Brown, M.Horoi, H.Grawe New T=1 effective interactions for the f5/2 p3/2 p1/2 g9/2 model space: Implications for valence-mirror symmetry and seniority isomers NUCLEAR STRUCTURE 58,60,62,64,66,68,70,72,74,76Ni, 80Zn, 82Ge, 84Se, 86Kr, 88Sr, 90Zr, 92Mo, 94Ru, 96Pd, 98Cd; calculated level energies. 70,72,74,76Ni, 92Mo, 94Ru, 96Pd, 98Cd; calculated transitions B(E2). New T=1 effective interactions. Comparisons with data.
doi: 10.1103/PhysRevC.70.044314
2004LI75 Phys.Rev. C 70, 064303 (2004) S.N.Liddick, P.F.Mantica, R.Broda, B.A.Brown, M.P.Carpenter, A.D.Davies, B.Fornal, T.Glasmacher, D.E.Groh, M.Honma, M.Horoi, R.V.F.Janssens, T.Mizusaki, D.J.Morrissey, A.C.Morton, W.F.Mueller, T.Otsuka, J.Pavan, H.Schatz, A.Stolz, S.L.Tabor, B.E.Tomlin, M.Wiedeking Development of shell closures at N = 32, 34. I. β decay of neutron-rich Sc isotopes RADIOACTIVITY 54,55,56Sc(β-) [from Be(86Kr, X)]; measured Eβ, Eγ, βγ-coin, T1/2. 54,55,56Ti deduced levels, J, π, configurations. Comparison with model predictions.
doi: 10.1103/PhysRevC.70.064303
2003HO04 Phys.Rev. C 67, 034303 (2003) M.Horoi, B.A.Brown, V.Zelevinsky Exponential convergence method: Nonyrast states, occupation numbers, and a shell-model description of the superdeformed band in 56Ni NUCLEAR STRUCTURE 52Cr, 56Ni; calculated single-particle configurations. 56Ni deduced superdeformed band features. Exponential convergence method.
doi: 10.1103/PhysRevC.67.034303
2003HO08 Phys.Rev. C 67, 054309 (2003) M.Horoi, J.Kaiser, V.Zelevinsky Spin- and parity-dependent nuclear level densities and the exponential convergence method
doi: 10.1103/PhysRevC.67.054309
2003HO18 Nucl.Phys. A718, 502c (2003) M.Horoi, R.Jora, V.Zelevinsky, A.St.J.Murphy, R.N.Boyd, T.Rauscher The 45V(p, γ) thermonuclear reaction rate relevant to 44Ti production rate in core-collapsed supernovae: a shell model analysis NUCLEAR REACTIONS 45V(p, γ), E=low; calculated astrophysical reaction rates. Shell model approach. NUCLEAR STRUCTURE 46Cr; calculated levels, J, π, spectroscopic factors. Shell model.
doi: 10.1016/S0375-9474(03)00870-4
2003MA02 Phys.Rev. C 67, 014311 (2003) P.F.Mantica, A.C.Morton, B.A.Brown, A.D.Davies, T.Glasmacher, D.E.Groh, S.N.Liddick, D.J.Morrissey, W.F.Mueller, H.Schatz, A.Stolz, S.L.Tabor, M.Honma, M.Horoi, T.Otsuka β decay studies of the neutron-rich 56-58V isotopes RADIOACTIVITY 56,57,58V(β-) [from Be(86Kr, X)]; measured Eγ, Iγ, βγ-, γγ-coin, T1/2; deduced log ft. 56,57,58Cr deduced levels, J, π. Systematics in neighboring isotones discussed. Comparison with model predictions.
doi: 10.1103/PhysRevC.67.014311
2003MA56 Phys.Rev. C 68, 044311 (2003) P.F.Mantica, B.A.Brown, A.D.Davies, T.Glasmacher, D.E.Groh, M.Horoi, S.N.Liddick, D.J.Morrissey, A.C.Morton, W.F.Mueller, H.Schatz, A.Stolz, S.L.Tabor β-decay properties of 55, 56Ti RADIOACTIVITY 55,56Ti(β-) [from Be(86Kr, X)]; measured β-delayed Eγ, Iγ, γγ-coin, T1/2; deduced β-branching ratios, role of spin-flip process. 55,56V deduced levels, feeding intensities. Comparisons with previous results, model predictions.
doi: 10.1103/PhysRevC.68.044311
2002HO03 Phys.Rev. C65, 027303 (2002) M.Horoi, B.A.Brown, V.Zelevinsky Applying the Exponential Convergence Method: Shell-model binding energies of 0f7/2 Nuclei Relative to 40Ca NUCLEAR STRUCTURE 42,43Sc, 44,45Ti, 46,47V, 48,49Cr, 50,51Mn, 52,53Fe, 54,55Co, 56Ni; calculated ground-state energies, J, π. Exponential convergence method, comparison with data.
doi: 10.1103/PhysRevC.65.027303
2002HO14 Phys.Rev. C66, 015801 (2002) M.Horoi, R.Jora, V.Zelevinsky, A.St.J.Murphy, R.N.Boyd, T.Rauscher 45V(p, γ) Thermonuclear Reaction Rate Relevant to 44Ti Production in Core-Collapse Supernovae: General Estimates and Shell Model Analysis NUCLEAR REACTIONS 45V(p, γ), E ≈ 0.1-2 MeV; calculated astrophysical S-factors, reaction rate, resonance contributions. Shell model analysis.
doi: 10.1103/PhysRevC.66.015801
2002HO16 Phys.Rev. C66, 024319 (2002) M.Horoi, A.Volya, V.Zelevinsky Random interactions, isospin, and the ground states of odd-A and odd-odd nuclei NUCLEAR STRUCTURE 20,21Ne, 21,22,23Na, 23,24,25Mg, 25,26,27Al, 27,28Si, 30P, 34Cl, 38K, 42Sc, 46V; calculated most probable spin, isospin quantum numbers for ground states. Random interaction model.
doi: 10.1103/PhysRevC.66.024319
2001HO27 Phys.Rev.Lett. 87, 062501 (2001) M.Horoi, B.A.Brown, V.Zelevinsky Random versus Realistic Interactions for Low-Lying Nuclear Spectra
doi: 10.1103/PhysRevLett.87.062501
1999HO05 Phys.Rev.Lett. 82, 2064 (1999) M.Horoi, A.Volya, V.Zelevinsky Chaotic Wave Functions and Exponential Convergence of Low-Lying Energy Eigenvalues NUCLEAR STRUCTURE 48Cr, 51Sc; calculated levels, J, π; deduced model convergence features, truncation criteria. Shell model, quantum chaotic many-body dynamics.
doi: 10.1103/PhysRevLett.82.2064
1996ZE05 Phys.Rep. 276, 85 (1996) V.Zelevinsky, B.A.Brown, N.Frazier, M.Horoi The Nuclear Shell Model as a Testing Ground for Many-Body Quantum Chaos
doi: 10.1016/S0370-1573(96)00007-5
1995HO05 Phys.Rev.Lett. 74, 231 (1995) Toward a Consistent Description of Parity Nonconservation in A = 18-21 Nuclei NUCLEAR STRUCTURE 18,19,20F, 21Ne; calculated parity nonconserving T=0, 1 matrix elements. Shell model.
doi: 10.1103/PhysRevLett.74.231
1995HO16 Phys.Rev.Lett. 74, 5194 (1995) M.Horoi, V.Zelevinsky, B.A.Brown Chaos vs Thermalization in the Nuclear Shell Model
doi: 10.1103/PhysRevLett.74.5194
1995ZE04 Phys.Lett. 350B, 141 (1995) V.Zelevinsky, M.Horoi, B.A.Brown Information Entropy, Chaos and Complexity of the Shell Model Eigenvectors
doi: 10.1016/0370-2693(95)00324-E
1994HO12 Phys.Rev. C50, 775 (1994) M.Horoi, G.Clausnitzer, B.A.Brown, E.K.Warburton New Calculations of the Parity Nonconservation Matrix Element for J(πT) 0+1, 0-1 Doublet in 14N NUCLEAR STRUCTURE 14N; calculated levels, B(λ), isoscalar parity nonconserving matrix element. Shell model.
doi: 10.1103/PhysRevC.50.775
1994HO13 Phys.Rev. C50, R2274 (1994) M.Horoi, B.A.Brown, V.Zelevinsky Truncation Method for Shell Model Calculations
doi: 10.1103/PhysRevC.50.R2274
1994HO14 Phys.Rev. C50, 2392 (1994) Parity Mixed Doublets in A = 36 Nuclei NUCLEAR STRUCTURE 36Cl, 36Ar; calculated levels, parity forbidden transitions γ CP, asymmetry. Different weak interactions, shell model with effective interactions.
doi: 10.1103/PhysRevC.50.2392
1994HO17 Phys.Rev. C50, 2834 (1994) Staggering of the Nuclear Charge Radii in a Superfluid Model with Good Particle Number NUCLEAR STRUCTURE 110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125Sn; calculated mean squared charge radii with, without deformation, neutron, proton pairing energies. Superfluid model, monopole pairing type 4-body interaction.
doi: 10.1103/PhysRevC.50.2834
1993GU11 J.Phys.(London) G19, 2063 (1993) R.K.Gupta, M.Horoi, A.Sandulescu, M.Greiner, W.Scheid Cluster Preformation Probabilities and Fine-Structure Effects in Heavy-Cluster Decays using Folding Potentials RADIOACTIVITY 221Fr, 225Ac, 221,222,223,224,226Ra(14C); calculated cluster decay width, Q, cluster preformation probability, other features. Double-folding potentials.
doi: 10.1088/0954-3899/19/12/011
1993HO14 Phys.Rev. C48, R522 (1993) Proposed New Experimental Case to Investigate the Weak Parity Nonconserving Couplings in 20F NUCLEAR STRUCTURE 20,19F; calculated parity nonconserving matrix elements; deduced parity nonconserving asymmetry estimate, possible experiment.
doi: 10.1103/PhysRevC.48.R522
1992SA30 Int.J.Mod.Phys. E1, 379 (1992) A.Sandulescu, R.K.Gupta, W.Greiner, F.Carstoiu, M.Horoi Role of Cluster Deformations on Their Preformation Probabilities in Radioactive Cluster-Decay Studies RADIOACTIVITY 230Th, 234,232U(24Ne); 222,224,226Ra(14C); 228Th(20O); 236Pu, 234U(28Mg); calculated cluster preformation probability, Gamow factors, WKB pentrabilities. Folded Michigan-3-Yukawa potential.
doi: 10.1142/S0218301392000199
1991BR28 Rev.Roum.Phys. 36, 135 (1991) I.Brandus, F.Carstoiu, O.Dumitrescu, M.Horoi, F.Nichitiu Multistep Direct and Compound Nuclear Reactions with Polarized Projectiles NUCLEAR REACTIONS 13C, 15N(p, p), (polarized p, p), E ≤ 1.17 MeV; calculated σ(θ), analyzing power vs E. Double-folding interaction potential, multi-step direct compound nuclear reactions.
1991KN03 Phys.Rev. C44, 491 (1991) N.Kniest, M.Horoi, O.Dumitrescu, G.Clausnitzer Isovector Parity Mixing in 16O Investigated via the 15N(p(pol), α0)12C Resonance Reaction NUCLEAR REACTIONS 15N(polarized p, α), E=resonance; analyzed data. 16O level deduced isovector parity mixing, α-decay features.
doi: 10.1103/PhysRevC.44.491
1990DU01 Phys.Rev. C41, 1462 (1990) O.Dumitrescu, M.Horoi, F.Carstoiu, G.Stratan Parity Nonconserving Asymmetries in Resonance Scattering and Nuclear Reactions Induced by Polarized Protons NUCLEAR REACTIONS 13C(polarized p, p), E=1.13-1.17 MeV; 15N(polarized p, p), E=0.6-0.8 MeV; calculated σ(E), analyzing power vs E. 15N(p, α), E not given; calculated parity nonconserving analyzing power.
doi: 10.1103/PhysRevC.41.1462
1990DU03 Nuovo Cim. 103A, 653 (1990) An Enlarged Superfluid Model of Atomic Nucleus NUCLEAR STRUCTURE 197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214Pb; calculated isotope shifts, rms charge radii. 152Sm; calculated levels. Enlarged superfluid model.
doi: 10.1007/BF02789018
1987AP02 Nucl.Phys. A470, 64 (1987) M.Apostol, I.Bulboaca, F.Carstoiu, O.Dumitrescu, M.Horoi Alpha-Like Four Nucleon Correlations in Superfluid Phases of Atomic Nuclei NUCLEAR STRUCTURE 152Nd, 156Sm, 160Gd, 164Dy, 168Er, 176Hf, 180W, 184Os, 240Pu, 246Cf; calculated coupling strength constants, gap parameters, mass differences, enhancement factors. BCS approach.
doi: 10.1016/0375-9474(87)90120-5
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